Light concentration apparatus, systems and methods

ABSTRACT

An optical device is disclosed including: a non-imaging secondary concentrator having an entry aperture and an exit aperture, and configured to receive light focused by a primary focusing element from a source onto the entry aperture. The non-imaging secondary concentrator includes: a first portion proximal the entry aperture which is rotationally symmetric about an optic axis; and a second portion proximal the exit aperture which is not rotationally symmetric about the optic axis.

CROSS REFERENCE TO RELATED APPLICATIONS

This application claims benefit of U.S. Provisional Application Ser. No. 61/230,083 filed Jul. 30, 2009, and to U.S. Provisional Application Ser. No. 61/230,485 filed Jul. 31, 2009. The entire contents of U.S. Provisional Application Ser. Nos. 61/230,083 and 61/230,485 are incorporated herein by reference.

BACKGROUND

The present disclosure relates generally to optical devices, and more particularly to optical systems incorporating non-imaging optical components.

Solar cells for electrical energy production are very well known but have limited utility due to the very high cost of production. For example, although substantial research has been ongoing for many years, the cost per Kilowatt-hour (Kwh) still is about ten times that of conventional electric power production. To compete with wind power or other alternative energy sources, the efficiency of production of electricity from solar cells should be drastically improved.

Therefore it is desirable to provide optical systems and methods that overcome the above and other problems. In particular, it is desirable to provide systems and methods that enhance the efficiency of collection of solar energy.

SUMMARY

The present disclosure provides systems and methods to concentrate light from a distant source, such as the sun, onto a target device, such as a solar cell.

Aspects of the present disclosure are directed to optical devices and systems that provide high solar flux onto a multi junction solar cell, or other target cell, to produce efficient electrical output.

According to one aspect, an optical device is provided that typically includes a primary focusing element, and a non-imaging secondary concentrator having an entry aperture and an exit aperture. Typically, the primary focus element is configured to focus light from a distant source onto the entry aperture of the secondary concentrator. In certain aspects, the primary focusing element has an f-number that is greater than about 1, e.g., between 1 and 4 or greater. In certain aspects, the device includes a solar cell located proximal to the exit aperture of the secondary concentrator. In certain aspects, the primary focusing element includes a Fresnel lens. In certain embodiments, the Fresnel lens is flat, substantially square (or other shape lacking rotational symmetry about the optical axis of the device), curved and/or refractive.

In another aspect, an optical device is disclosed including: a non-imaging secondary concentrator having an entry aperture and an exit aperture, and configured to receive light focused by a primary focusing element from a source onto the entry aperture. The non-imaging secondary concentrator includes: a first portion proximal the entry aperture which is rotationally symmetric about an optic axis; and a second portion proximal to the exit aperture which is not rotationally symmetric about the optic axis.

Some embodiments include a receiver located proximal to the exit aperture of the secondary concentrator. In some embodiments, the receiver is optically coupled to the exit aperture of the secondary concentrator.

In some embodiments, the second portion extends and tapers along the optic axis from a wide end proximal to the first portion to a narrow end including the exit aperture.

In some embodiments, the shape of the exit aperture corresponds to the shape of the receiver.

In some embodiments, the receiver is square shaped, and the second portion of the non-imaging secondary concentrator includes a truncated substantially square pyramidal portion extending which extends and tapers along the optic axis from a wide end proximal the first portion to a narrow end including the exit aperture.

In some embodiments, the non-imaging secondary concentrator is composed of a transparent dielectric material.

In some embodiments, the non-imaging secondary concentrator operates by total internal reflection.

In some embodiments, the non-imaging secondary concentrator operates by both total internal reflection and specular reflection.

In some embodiments, the secondary concentrator includes a compound parabolic concentrator (CPC).

In some embodiments, the first portion of the non-imaging secondary concentrator includes a spherical or aspheric-shaped entrance aperture.

In some embodiments, the secondary concentrator includes an angle transformer.

Some embodiments include the primary focusing element.

In some embodiments, the primary focusing element has an f-number that is greater than about 0.9, or greater than about 1.5.

In some embodiments, the primary focusing element includes a Fresnel lens. In some embodiments, the Fresnel lens is flat. In some embodiments, the Fresnel lens is substantially square. In some embodiments, the Fresnel lens is curved. In some embodiments, the Fresnel lens is refractive.

Some embodiments include a means for homogenizing the light focused onto the entry aperture of the secondary concentrator.

In some embodiments, the primary focusing element includes a diffractive lens, a reflector, or a Fresnel reflector.

In some embodiments, the receiver includes an energy converting element adapted to absorb light and output energy in response to the absorbed light.

In some embodiments, the energy converting element outputs electrical energy in response to the absorbed light.

In some embodiments, the energy converting element includes a photovoltaic cell, or a multi junction photovoltaic cell.

In some embodiments, the energy converting element produces thermal energy in response to the concentrated light.

In another aspect, a method is disclosed including: providing a non-imaging secondary concentrator having an entry aperture and an exit aperture; where the non-imaging secondary concentrator includes: a first portion proximal the entry aperture which is rotationally symmetric about the optic axis; a second portion proximal the exit aperture which is not rotationally symmetric about the optic axis. The method also includes receiving light focused by a primary focusing element from a source onto the entry aperture; concentrating light onto a receiver located proximal to the exit aperture of the secondary concentrator; and absorbing light concentrated on the receiver and outputting thermal or electrical energy in response to the absorbed light.

In another aspect, an apparatus is disclosed for concentrating light from a source including: a truncated tapered reflector extending along an optic axis from a wide end to a narrow end and defining an interior region; and a concentrating lens mounted in the wide end of the reflector, the lens having a central region disposed about the optic axis and a peripheral region disposed about the central region. The narrow end of the truncated tapered reflector is adapted to mount a receiver, and the concentrating lens is adapted to receive light from the source and concentrate light through the interior region and onto the receiver.

In some embodiments, a portion of the light from the source passing through the central region of the concentrating lens is directed to the receiver without reflecting from the reflector. A portion of the light from the source passing through the peripheral region of the concentrating lens is reflected from a surface of the reflector facing the interior region and onto the receiver.

In some embodiments, the concentrator lens includes a Fresnel lens.

In some embodiments, the truncated tapered reflector is a truncated substantially reflector having a round aperture at the wide end, and the concentrating lens is a round lens mounted in the round aperture.

In some embodiments, the truncated tapered reflector is a truncated substantially square pyramidal reflector having a square aperture at the wide end, and the concentrating lens is a square lens mounted in the square aperture.

Some embodiments include the receiver mounted at the narrow end of the reflector.

In some embodiments, the interior region includes a sealed volume. In some embodiments, the sealed volume includes an evacuated volume. In some embodiments, the sealed volume contains a refractive material.

In some embodiments, the refractive material includes a fluid. Some embodiments include a fluid exchange system in fluid communication with the sealed volume and configured to circulate the fluid through the volume. Some embodiments including a heat exchanger configured to extract heat from the circulating fluid.

In some embodiments, concentrating lens is a comatic lens which is adapted to be substantially free from ray crossing at points about the optic axis proximal the narrow end of the reflector. In some embodiments, the concentrating lens is characterized in that, in the absence of the reflector, each pair light rays entering the lens parallel to the optic axis and at differing radial distances from the optic axis are directed without crossing to a plane extending transverse the optic axis at a position corresponding to the position of the receiver at the narrow end of the reflector.

In some embodiments, the concentrating lens has an f-number of 2 or less, of 1 or less, of 0.75 or less, or of 0.5 or less.

In some embodiments, light from the source incident on the concentrating lens at an angle of incidence less than about 1.5 degrees from the optic axis is concentrated to the receiver with an efficiency of greater than about 70%, 80%, 85%, or more.

In some embodiments, light from the source incident on the front surface at an angle of incidence less than about 2 degrees is concentrated to the receiver with a geometrical concentration ratio of about 500 or greater, about 600 or greater, about 800 or greater, or more.

Some embodiments include the source. In some embodiments, the source includes a light emitting diode; an organic light emitting diode, a laser; and a lamp.

In some embodiments, the receiver includes an energy converting element adapted to absorb light and output energy in response to the absorbed light.

In some embodiments, the energy converting element outputs electrical energy in response to the absorbed light. In some embodiments, the energy converting element includes a photovoltaic cell. In some embodiments, the energy converting element includes a multi junction photovoltaic cell.

In some embodiments, the energy converting element produces thermal energy in response to the concentrated light.

In some embodiments, the receiver includes a photodiode, a laser gain medium, or a photographic medium.

In some embodiments, the receiver includes a digital imaging sensor. In some embodiments, the digital imaging sensor included is of at least one element selected from the group consisting of: a CCD, a multi-pixel array of photodetectors, a CMOS detector.

In some embodiments, the receiver includes a digital light processor or a MEMs device.

In some embodiments, the receiver includes a light emitting element, and where the reflector and the concentrated lens cooperate to collect emitted light from the light emitting element and form a beam of emitted light which is output from the wide end of the reflector. In some embodiments, the beam is substantially collimated.

In some embodiments, the light emitting element includes a light emitting diode, an organic light emitting diode, a laser, or a lamp.

In some embodiments, the source is the sun.

In another aspect, a method is disclosed including: providing a concentrator which includes a truncated tapered reflector extending along an optic axis from a wide end to a narrow end and defining an interior region; a concentrating lens mounted in the wide end of the reflector, the lens having a central region disposed about the optic axis and a peripheral region disposed about the central region; and a receiver mounted in the narrow end of the reflector. The method also includes using the concentrating lens to receive light from the source and concentrate light through the interior region and onto the receiver.

In some embodiments, using the concentrating lens to receive light from the source and concentrate light through the interior region and onto the receiver includes: passing a first portion of the light from the source through the central region of the concentrating lens to direct the first portion to the receiver without reflecting from the reflector; passing a second portion of the light from the source through the peripheral region of the concentrating lens to direct the second portion to the reflector; and reflecting the second portion from a surface of the reflector facing the interior region and onto the receiver.

In some embodiments, the concentrator lens includes a Fresnel lens.

In some embodiments, the truncated tapered reflector is a truncated conical reflector having a round aperture at the wide end, and the concentrating lens is a round lens mounted in the round aperture.

In some embodiments, truncated tapered reflector is a truncated square pyramidal reflector having a square aperture at the wide end, and where the concentrating lens is a square lens mounted in the square aperture.

In another aspect, an apparatus is disclosed for concentrating light from a source which includes a truncated trough shaped reflector. The reflector extends along a longitudinal axis, and extends and tapers along a latitudinal axis from a wide end to a narrow end. The trough defines an interior region divided by an optic plane extending along the longitudinal and latitudinal axes. Also included are a concentrating lens mounted in the wide end of the reflector extending along the longitudinal axis and transverse the optic plane, the lens having an inner region proximal the optic plane and one or more outer regions distal the optic plane. The narrow end of the conical reflector is adapted to mount a receiver; and the concentrating lens is adapted to receive light from the source and concentrate light through the interior region and onto the receiver.

In some embodiments, a portion of the light from the source passing through the inner region of the concentrating lens is directed to the receiver without reflecting from the reflector; and a portion of the light from the source passing through the one or more outer regions of the concentrating lens is reflected from a surface of the reflector facing the interior region and onto the receiver.

In some embodiments, the concentrator lens includes a Fresnel lens.

In some embodiments, light from the source incident on the concentrating lens at an angle of incidence within at least about 1 degree from normal to the lens in a direction transverse the optic plane and within at least about 20 degrees from normal to the lens in the longitudinal direction is concentrated to the concentration region with an efficiency of greater than about 85%.

In some embodiments, light from the source incident on the concentrating lens at an angle of incidence within at least about 1 degree from normal to the lens in a direction transverse the optic plane and within at least about 20 degrees from normal to the lens in the longitudinal direction is concentrated on the receiver with a geometrical concentration ratio of about 10 or greater.

In another aspect, an apparatus for concentrating light from a source is disclosed including: a truncated tapered reflector extending along an optic axis from a wide end to a narrow end and defining an interior region; and a concentrating lens mounted in the wide end of the reflector. The narrow end of the conical reflector is adapted to mount a receiver. The concentrating lens is adapted to receive light from the source and concentrate light through the interior region and onto the receiver. A first portion of the light from the source passing through the concentrating lens is directed to the receiver without reflecting from the reflector. A second portion of the light from the source passing through concentrating lens is reflected from a surface of the reflector facing the interior region and onto the receiver.

In another aspect, an apparatus for concentrating light from a source is disclosed including: a truncated trough shaped reflector which extends along a longitudinal axis and extends and tapers along a latitudinal axis from a wide end to a narrow end. The trough defines an interior region divided by an optic plane extending along the longitudinal and latitudinal axes. A concentrating lens mounted in the wide end of the reflector extending along the longitudinal axis and transverse the optic plane. The narrow end of the conical reflector is adapted to mount a receiver. The concentrating lens is adapted to receive light from the source and concentrate light through the interior region and onto the receiver. A first portion of the light from the source passing through the concentrating lens is directed to the receiver without reflecting from the reflector. A second portion of the light from the source passing through concentrating lens is reflected from a surface of the reflector facing the interior region and onto the receiver.

Various embodiments may include any of the above described features, either alone, or in combination.

As used herein, the f-number of an optical element is defined as one half times the inverse of the numerical aperture NA of the element. For an optical element having an acceptance angle θ, and working in a media having an index of refraction n, the numerical aperture is given by NA=n sin θ.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates an optical device.

FIG. 2A is a side view of a rotationally symmetric secondary concentrator.

FIG. 2B is a perspective view of a rotationally symmetric secondary concentrator.

FIG. 2C is a perspective view of a secondary concentrator featuring a rotationally asymmetric portion.

FIG. 3 is a plot of optical efficiency vs. angle of incidence for two types of secondary concentrators.

FIGS. 4 a-4 c are irradiance plots for a target illuminated by rotationally symmetric secondary concentrator.

FIGS. 5 a-5 d are irradiance plots for a target illuminated by a secondary concentrator featuring a rotationally asymmetric portion.

FIG. 6 is a cross section of a concentrator.

FIG. 6 a is a cross section of a concentrator.

FIG. 7 is a ray trace illustration for a concentrating lens with inset showing detail.

FIG. 8 is a ray trace illustration for a concentrating lens with inset showing detail.

FIG. 9 is ray trace illustration for a concentrating Fresnel lens with inset showing detail.

FIG. 10 is ray trace illustration for a concentrating Fresnel lens with inset showing detail.

FIG. 11 a-c illustrate a three dimensional concentrator with a circular concentrating lens. FIG. 11 a is a perspective view. FIG. 11 b is a ray trace illustration. FIG. 11 c is a cross section.

FIG. 12 is a chart of characteristics of the concentrator of FIGS. 11 a-c.

FIG. 13 is a plot of optical efficiency vs angle of incidence for the concentrator of FIGS. 11 a-c.

FIGS. 14 a-b illustrate a three dimensional concentrator with a square concentrating lens.

FIG. 15 is a chart of characteristics of the concentrator of FIGS. 11 a-c and the concentrator of FIGS. 14 a-b.

FIG. 16 is a plot of optical efficiency vs angle of incidence for the concentrator of FIGS. 11 a-c and the concentrator of FIGS. 14 a-b.

FIGS. 17 a and 17 b illustrate and compare the irradiance patterns for the concentrator of FIGS. 11 a-c and the concentrator of FIGS. 14 a-b.

FIG. 18 a-b illustrate a two dimensional concentrator with a trough shaped reflector. FIG. 18 a is a perspective view, FIG. 18 b is a cross section.

FIG. 19 is a chart of characteristics of the concentrator of FIGS. 18 a-b.

FIG. 20 shows plots of the optical efficiency vs angle of incidence for the concentrator of FIGS. 18 a-b.

FIGS. 21 a-21 d show a listing of a SciLab script of an exemplary optical design method.

DETAILED DESCRIPTION

The present disclosure provides systems and methods to concentrate light from a distant source, such as the sun, onto a target device, such as a solar cell.

According to one embodiment, an optical device 10 includes a primary focusing element 20, and a non-imaging secondary concentrator 30 having an entry aperture 35 and an exit aperture 40. In one aspect, the primary focusing element 20 is configured to focus light from a distant source onto the entry aperture 35 of the secondary concentrator 30. Light received at the entry aperture 35 is provided to an exit aperture 40. In one aspect a target device 45 such as a solar cell is located proximal to the exit aperture 40 to receive the concentrated light. The target device 45 may be located above or below a plane defining the exit aperture or it may be located substantially on the plane, or it may be optically coupled with the exit aperture.

In certain aspects, the primary focusing element 20 includes a lens element that has an f-number that is greater than about 1, e.g., between 1 and 4 or even greater. One example of a useful primary focusing element 20 is a substantially flat and square Fresnel lens. Other useful primary focusing elements include curved Fresnel lenses, non-square, flat Fresnel lenses, a Fresnel reflector, any focusing lens, a diffractive lens, a reflective element such as a mirror, a holographic lens element, or any other optical element that focuses or redirects light. In one aspect, a flat cover 22, e.g., made of glass or PMMA or other suitable optically transparent material, is positioned on or proximal to the primary focusing element on a side opposite the non-imaging secondary concentrator. Cover 22 provides additional environmental protection for the primary focusing element 20 or any other optical element, and allows the primary focusing element 20 to be very thin, e.g., a very thin layer.

In certain aspects, the device 10 also includes a means for homogenizing the light focused onto the entry aperture of the secondary concentrator. Examples of homogenizing elements or systems include Kohler homogenizers, holographic devices, kaleidoscopes, etc. U.S. patent application Ser. No. 11/683,934, filed Mar. 8, 2007, illustrates useful homogenizing elements and is incorporated herein by reference in its entirety. Also, U.S. patent application Ser. No. 11/084,882, filed Mar. 21, 2005, illustrates useful concentrator elements and other optical device features and is incorporated herein by reference in its entirety.

In certain aspects, the non-imaging secondary concentrator 30 is composed of a transparent dielectric material. In certain aspects, the non-imaging secondary concentrator 30 includes a compound parabolic concentrator (CPC), or a θ_(i)/θ_(o) angle transformer, or a flow line concentrator. For example, the secondary concentrator 30 may be made of a transparent dielectric material and may include a spherical or aspheric-shaped entrance aperture and a planar exit aperture. It should be appreciated that any concentrator element can be used. For example, the non-imaging secondary concentrator, in certain aspects, may operate by total internal reflection (TIR) and/or specular reflection. The region between the primary focusing element 20 and the concentrator 30 may be composed of air (n=1) or a solid transparent dielectric material having a different index of refraction than the concentrator, e.g., between 1 and 3, or greater. A liquid medium having a different index of refraction than the concentrator may also be used, in which case a body structure is included to hold the primary focusing element and concentrator and the liquid medium.

In certain aspects, the device advantageously has an optical acceptance angle of about 5 degrees or greater with an optical efficiency of between about 80-85%. In certain aspects, the devices of the present invention provide a uniform flux distribution on the target (e.g., solar cell) and are suitable for use with multi junction (MJ) and Si target cells, among others. In one specific embodiment, for example, a device might be configured with a 125 mm×125 mm entry aperture, a depth of about 230 mm. Solar cell sizes for this embodiment might include a 5.5 mm×5.5 mm MJ cell or a 10 mm×10 mm Si cell. This would provide a geometric concentration of about 500 for the MJ cell or about 150 for the Si cell, with acceptance angles of about 30 degrees for the MJ cell or 5 degrees for the Si cell, and an optical efficiency of between about 80-85%.

It should be appreciated that target 45 may include a light source or an illumination element, in which case the optical system operates as an illuminator.

According to one embodiment, a heat sink 50 is provided on which to mount one or more optical systems. The heat sink may include a U-beam structure or comb structure as is well known, however other structures may be used as desired. The heat sink may also provide a platform on which to mount multiple systems. The target cell may be attached directly to the heat sink, or a heat spreader (e.g., Aluminum Nitride) may be provided to couple the heat sink with the target and enhance heat dissipation from the cell to the heat sink. In certain aspects, a tracking system is provided to reposition the system(s) as needed to track the motion of the sun and maintain the light impinging on the system within a desirable acceptance angle.

FIGS. 2 a and 2 b show one embodiment 30 a of concentrator 30 which includes a spherical top portion 60 which includes entrance aperture 35. Concentrator 30 a also includes a bottom cylindrical tapering portion 70 which includes circular exit aperture 40 for concentrating light onto the target cell 45. Both portions of concentrator 30 a are rotationally symmetric about optic axis O.

FIG. 2C shows an alternate embodiment 30 b of concentrator 30 which includes a spherical top portion 60 which includes entrance aperture 35. This top portion is similar to the top portion of concentrator 30 a. However, concentrator 30 b includes a bottom tapering portion 80 which includes square exit aperture 40 b for concentrating light onto the target cell 45. Thus concentrator 30 b includes a top portion 60 which is rotationally symmetric about optic axis O, and a bottom portion 80 which in not rotationally symmetric.

Note that, in other embodiments, bottom portion 80 may terminate in exit apertures having other shapes, e.g. a triangle, a regular polygon, an irregular shape, etc.

FIG. 3 shows a plot of optical efficiency vs acceptance angle for concentrator 30 a with a circular exit aperture and concentrator 30 b with a square exit aperture. The results are substantially identical for both concentrators 30 a and 30 b. However, the distribution of irradiance at target cell 45 differs between the concentrators 30 a and 30 b.

For example, FIGS. 4 a-4 c show plots of the irradiance of target cell 45 using concentrator 30 a for light incident at 0 degrees, 0.8 degrees and 1.4 degrees, respectively. Note that in FIGS. 4 a and 4 b, the irradiance is strongest at the center of the target.

FIGS. 5 a-d show plots of the irradiance of target cell 45 using concentrator 30 b for light incident at 0 degrees, 0.8 degrees, 0.8 degrees and 1.4 degrees, respectively. In FIG. 5 b, the angle is in a direction parallel to a side of the square exit aperture. In FIGS. 5 c and 5 d, the angle is in a direction parallel to the diagonal of the square aperture. Note that, for concentrator 30 b the irradiance of target cell 45 is less peaked at the center of the cell. For example, in some embodiments, the ratio of the peak concentration on the cell to the average concentration over the cell may be 5.0 or less, 4.0 or less, 3.0 or less, 2.0 or less, or even about 1.0 (corresponding to uniform illumination.)

Thus, concentrator 30 b may be used advantageously in application where it is beneficial to “spread out” the irradiance more uniformly across target cell 45. As is known in the art, many types of solar cells and other optical devices operate more efficiently when uniformly illuminated. For example, a typical solar cell may be suitable for use at concentrations of, e.g. up to C=500. However, in some applications even though the average concentration on the cell is below this limit, when such a device is illuminated non-uniformly, e.g. such that solar light is concentrated to localized portions of the cell at concentrations significantly greater than C=500. This uneven concentration can lead to localized regions of high temperature on the cell, leading to degraded performance and possible damage. In addition, ultra-high solar flux can cause electric breakdown of tunnel diode layers between junctions of a multi junction cell degrading performance.

Notably, concentrator 30 b may provide the advantageous uniform distributions described above with a relatively simple shape and compact form factor. For example, in some embodiments, concentrator 30 b has a shape suitable for fabrications using molding techniques known in the art. For example, the concentrator may be fabricated by flowing molten glass into a form and allowing the glass to cool and solidify. In some embodiments (e.g., for relatively low temperature concentration applications), the concentrator can be molded from acrylic, plastic, or other suitable material. In some embodiments the concentrator may be relatively short, e.g. characterized by an f-number of 2 or less, 1 or less, 0.5 or less, etc.

A person skilled in the art will appreciate that these features represent advantages over conventional optical mixers. Such mixers are typically refractive elements which are rotationally asymmetric about an optical axis. These devices receive light at an entrance face, mix incoming light using a multiple successive TIR (total internal reflection) reflections from lateral surfaces of the mixer, and output light with a more uniform distribution from an exit face. Typically, these mixers have complicated shapes which cannot be fabricated using molding techniques, requiring instead more complicated and costly fabrication techniques such as precision grinding. Moreover, these mixers are typically very long, and cannot be used in high concentration systems (e.g., systems which provide concentration at or near the thermodynamic limit) while maintaining a small f-number (e.g. less that 0.5, less than 1.0, less than 2.0, etc.). Further, because the reliance on multiple TIR reflections, mixers of this type are often susceptible to performance degradation due to debris on or damage to the mixer's lateral surface.

Concentrator 30 b may include any of the features described above. Various embodiments of concentrator 30 b can be designed and tailored for a given application using techniques known in the art. For example, FIGS. 21A-D contain an exemplary script for generating the design of a concentrator of the type described above in the well known SciLab scientific computing environment (available at “http://www.scilab.org”).

Lens-Mirror Concentrator

In another aspect of this disclosure, embodiments of concentrators featuring a lens (e.g. fast lenses having a low f-number, e.g. lower than 2, lower than 1, lower than 0.9, lower than 0.75, or lower than 0.5 or less) paired with a reflective mirror surface to concentrate light onto a receiver.

Referring to FIG. 6, concentrator 100 includes concentrating lens 101 mounted in the wide end of tapering reflector 102. Receiver 103 (in this example a photovoltaic cell) is mounted at the narrow end of the reflector 102. Thus, the interior volume 104 of reflector 101 is sealed, protecting receiver 103. Interior volume 104 may be evacuated, or may be filled with a fluid (e.g. a transparent refractive fluid) or solid (e.g. a solid refractive dielectric). In cases where interior volume 104 is filled with a fluid, a circulator (not shown) may be provided in fluid communication (e.g. through one or more ports in reflector 102) with interior volume 104. The circulator may circulate the fluid to remove heat from concentrator 100. It may further include a heat exchanger which extracts heat from the circulating fluid. This heat may be used, e.g., to generate electrical power, generate steam power, provide home heating, etc.

As indicated by the ray traces in FIG. 6, a first portion of the light passing through lens 101 is refracted and directed to receiver 103 without reflecting from reflector 102. A second portion of the light passing through lens 101 is refracted and reflects from reflector 102 onto receiver 103.

For example, as shown in FIG. 6, rays which enter the central portion of lens 101 at relatively small angle of incidence from normal incidence make up the first portion of light which impinges directly on cell 103. Rays which enter the peripheral portion of lens 101 and/or are incident at relatively large angle of incidence from normal make up the second portion of light which reflects from reflector 102 before impinging on receiver 103.

FIG. 6 a is an illustration of concentrator 100 only showing light rays belonging to the second portion of light, which reflects from reflector 102 before impinging on receiver 103. Note that the rays 105 a and 105 b are reflected onto the edges of receiver 103, while the remaining rays are directed to points on receiver 103 between the edges. The rays illustrated reflect off one side of reflector 102, but of course a symmetric set of rays could be drawn which reflect off of the opposite side.

In some embodiments, concentrator 100 is advantageous in that it can provide good performance while being much shorter than conventional concentrators, e.g., compound parabolic concentrators (CPCs).

In some embodiments, concentrating lens 101 may be a singlet lens. As is known in the art, fast singlet lens often have coma. For example, FIG. 7 is a ray trace of a typical fast singlet concentrating lens. Note that, as shown, reflector 102 is not present in the figure. The plane 201 corresponds to the desired location of receiver 103. However, as detailed in the inset, the coma of lens 101 results in ray crossings which occur in front of the receiver plane. Rays which cross in this fashion cannot be suitably concentrated by a reflector to the receiver 103 in receiver plane 201. The reason for this is that a mirror cannot reflect two rays which have already crossed to a single point.

In some embodiments, a slow lens having low coma can be used to avoid the problem of ray crossing. However, typically such designs will require a longer concentrator than those featuring a fast lens. FIG. 8 illustrates another solution to the ray crossing problem that does not require a slow, substantially coma-free lens. As shown, lens 101 is designed in such a way that rays cross the receiver plane incrementally, i.e., incident rays with smaller y coordinates (vertical direction in the figure) cross the points with smaller y value on the receiver plane. Thus although coma still exists and may be large, no rays cross before the receiver plane. Accordingly, the rays can be well concentrated by reflector 102.

Conventional fast lenses may be thick and bulky, and may require a lot of material and be difficult to manufacture. Accordingly, in some embodiments, lens 101 may be constructed as a Fresnel lens. Advantageously, Fresnel lenses may be thinner and require less material than conventional lenses. FIGS. 9 and 10 show ray traces of exemplary Fresnel lenses suitable for use in concentrator 100. Note that in each case, ray crossing in front of receiver plane 103 is minimized or eliminated.

In some embodiments, concentrator 100 is a three dimensional concentrator with high geometric concentration (e.g. geometric concentration of 100, 500, 1000, or more). For example, FIGS. 11 a-c illustrate an embodiment of concentrator 100 which is rotationally symmetric about optic axis O. Lens 101 is a circular lens, and reflector 102 is a truncated substantially conical surface. Exemplary dimensions for one embodiment are shown in FIG. 11 c, but it is to be understood that other dimensions may be used.

Referring to FIGS. 12 and 13, the embodiment of concentrator 100 shown in FIGS. 11 a-c may have a geometric concentration of 820 with an acceptance angle of 1.5 degrees or more. Concentrator 100 operates with an optical efficiency of 85% or more for light incident at angles less than the acceptance angle. Other embodiments may have other performance characteristics. In some embodiments, the geometric concentration may be greater than 500, greater than 750, greater than 1000, or even more. The optical efficiency may be greater than 70%, 80%, 90%, or more. The acceptance angle may be greater than 1 degree, 1.5 degrees, 2.0, degrees or more.

FIGS. 14 a-b illustrate an embodiment of concentrator 100 featuring a three dimensional square pyramidal geometry. Lens 101 is a square lens, and reflector 102 is a truncated substantially square pyramidal surface. Referring to FIGS. 15 and 16, the performance of this square concentrator is comparable to that of the circular concentrator of FIGS. 11 a-c.

The embodiment of concentrator 100 shown in FIGS. 14 a-b may have a geometric concentration of 820 with an acceptance angle of about 1.0 degrees or more. Concentrator 100 operates with an optical efficiency of about 84% or more for light incident at angles less than the acceptance angle. For example, FIG. 16 shows the optical efficiency of the concentrators as a function of angle of incidence. In the case of the square concentrator, efficiency is plotted for angles along the direction of a side of square lens 100 and in the direction along the diagonal of square lens 100.

Other embodiments of the square concentrator may have other performance characteristics. In some embodiments, the geometric concentration may be greater than 500, greater than 750, greater than 1000, or even more. The optical efficiency may be greater than 70%, 80%, 90%, or more. The acceptance angle may be greater than 1 degree, 1.5 degrees, 2.0, degrees or more.

FIGS. 17 a and 17 b compare the irradiance pattern produced at receiver 103 for the circular concentrator of FIGS. 11 a-c and the square concentrator of FIGS. 14 a-b. Note that for the square concentrator, the irradiance of receiver 103 is less peaked at the center of the cell. Thus, square concentrator may be used advantageously in application where it is beneficial to “spread out” the irradiance more uniformly across receiver 103. For example, in some embodiments, for the square concentrator (or a similar concentrator using another shape which is rotationally asymmetric about the optic axis), the ratio of the peak concentration on the cell to the average concentration over the cell may be 5.0 or less, 4.0 or less, 3.0 or less, 2.0 or less, or even about 1.0 (corresponding to uniform illumination). As is known in the art, many types of solar cells and other optical devices operate more efficiently when uniformly illuminated.

Although specific examples of circular and square three dimensional high concentration concentrators have been discussed, it is to be understood that, in various embodiments, any other suitable shapes may be used.

In some embodiments, these concentrators may be used, e.g., in solar collection applications where they are mounted on a solar tracking system of any kind known in the art.

In some embodiments, concentrator 100 is a two dimensional concentrator with low geometric concentration (e.g., geometric concentration of 20 or less, 10 or less, 5 or less, etc.). For example, FIGS. 18 a and 18 b show concentrator 100, in which reflector 102 is a trough shaped reflector which extends along a longitudinal axis A (e.g. for 100 mm or less or more) and tapers vertically from a wide top to a narrow bottom. For solar collection applications, longitudinal axis A may be arranged along a North-South direction.

Concentrating lens 101 is a cylindrical type lens which extends along axis A, and is mounted in the wide top of trough shaped reflector 102. Concentrator 100 acts to concentrate light to an elongated region extending along the narrow bottom of the trough. Receiver 103 is positioned in or near this elongated region, and may also extend along the longitudinal axis, as shown.

Referring to FIGS. 19 and 20, the embodiment of concentrator 100 shown in FIGS. 18 a-b may have a geometric concentration of 14 with an acceptance angle of 23 degrees or more along the longitudinal direction (indicated as N.S. in the figures) and of 2.6 degrees in the lateral direction (i.e. transverse to the plane or symmetry of the trough, indicated as E.W in the figures). Concentrator 100 operates with an optical efficiency of 87.6% or more for light incident at angles less than the acceptance angle.

Other embodiments may have other performance characteristics. In some embodiments, the geometric concentration may be greater 5, greater than 10, or even more. The optical efficiency may be greater than 70%, 80%, 90%, or more. The acceptance angle may be greater than 1 degree, 2 degrees, 3, degrees or more in the longitudinal direction.

In some embodiments, light from a source incident on the concentrating lens 101 at an angle of incidence within at least about 1 degree from normal to the lens in the lateral direction and within at least about 20 degrees from normal to the lens in the longitudinal direction is concentrated to the concentration region with an efficiency of greater than about 85% and with an geometrical concentration ratio of about 10 or greater.

Note that, because the two dimensional concentrator generally has a wider acceptance angle than a high concentration device, it may be more suitable in solar collection applications where no or limited tracking is available.

Reflector 102 may be formed, e.g., from stamped metal such as aluminum (or any other metal suitable for forming a reflective surface.). In other embodiments reflector 102 is formed as a metallized coating on a refractive material (e.g. a coating including gold or silver or aluminum, or any other reflective coating known in the art.). In some embodiments, some or all of reflector 102 may operate by total internal reflection.

Although the specific examples described above have dealt with concentrating radiation from a relatively large solid angle of incidence onto a relatively small target (e.g. concentrating solar light onto a solar cell), it will be understood that they may equally well be applied to broadcasting radiation from a relatively small source to a relatively large solid angle (e.g. collecting light from an LED chip to form a beam or sheet of light). The small source may, for example, include a light emitting diode, an organic light emitting diode, a laser, or a lamp.

One or more or any part thereof of the techniques described herein can be implemented in computer hardware or software, or a combination of both. The methods can be implemented in computer programs using standard programming techniques following the method and figures described herein. Program code is applied to input data to perform the functions described herein and generate output information. The output information is applied to one or more output devices such as a display monitor. Each program may be implemented in a high level procedural or object oriented programming language to communicate with a computer system. However, the programs can be implemented in assembly or machine language, if desired. In any case, the language can be a compiled or interpreted language. Moreover, the program can run on dedicated integrated circuits preprogrammed for that purpose.

Each such computer program is preferably stored on a storage medium or device (e.g., ROM or magnetic diskette) readable by a general or special purpose programmable computer, for configuring and operating the computer when the storage media or device is read by the computer to perform the procedures described herein. The computer program can also reside in cache or main memory during program execution. The analysis method can also be implemented as a computer-readable storage medium, configured with a computer program, where the storage medium so configured causes a computer to operate in a specific and predefined manner to perform the functions described herein. In some embodiments, the computer readable media is tangible and substantially non-transitory in nature, e.g., such that the recorded information is recorded in a form other than solely as a propagating signal.

Note that as used herein, an acceptance angle should be taken as symmetric about zero, i.e., a device with an acceptance angle of 5 will accept light rays at angles ranging from −5 degrees to +5 degrees.

A number of embodiments of the invention have been described. Nevertheless, it will be understood that various modifications may be made without departing from the spirit and scope of the invention.

As used herein the term “light” and related terms (e.g. “optical”) are to be understood to include electromagnetic radiation both within and outside of the visible spectrum, including, for example, ultraviolet and infrared radiation.

In general, concentrators of the type described herein may be designed by appropriate application of the “edge-ray” principal, e.g., as described in Roland Winston et al, Nonimaging Optics, Academic Press (Elsevier) 2005.

U.S. patent application Ser. No. 12/036,825 filed Feb. 25, 2008, and U.S. Provisional Application Ser. No. 60/891,447 filed Feb. 23, 2007, are incorporated herein by reference in their entirety.

Having thus described several aspects of at least one embodiment of this invention, it is to be appreciated that various alterations, modifications, and improvements will readily occur to those skilled in the art. Such alterations, modifications, and improvements are intended to be part of this disclosure, and are intended to be within the spirit and scope of the invention. Accordingly, the foregoing description and drawings are by way of example only. 

1. An optical device, comprising: a non-imaging secondary concentrator having an entry aperture and an exit aperture, and configured to receive light focused by a primary focusing element from a source onto the entry aperture; wherein the non-imaging secondary concentrator comprises: a first portion proximal the entry aperture which is rotationally symmetric about an optic axis; a second portion proximal the exit aperture which is not rotationally symmetric about the optic axis.
 2. The device of claim 1, further comprising a receiver located proximal to the exit aperture of the secondary concentrator.
 3. The device of claim 2, wherein the receiver is optically coupled to the exit aperture of the secondary concentrator.
 4. The device of claim 2, wherein the second portion extends and tapers along the optic axis from a wide end proximal the first portion to a narrow end comprising the exit aperture.
 5. The device of claim 4, wherein the shape of the exit aperture corresponds to the shape of the receiver.
 6. The device of claim 5, wherein the receiver is square shaped, and the second portion of the non-imaging secondary concentrator comprises a truncated substantially square pyramidal portion, which extends and tapers along the optic axis from a wide end proximal the first portion to a narrow end comprising the exit aperture.
 7. The device of claim 1, wherein the non-imaging secondary concentrator is composed of a transparent dielectric material.
 8. The device of claim 7, wherein the non-imaging secondary concentrator operates by total internal reflection.
 9. The device of claim 8, wherein the non-imaging secondary concentrator operates by both total internal reflection and specular reflection.
 10. The device of claim 1, wherein the secondary concentrator includes a compound parabolic concentrator (CPC).
 11. The device of claim 10, wherein the first portion of the non-imaging secondary concentrator comprises a spherical or aspheric-shaped entrance aperture.
 12. The device of claim 1, wherein the secondary concentrator includes an angle transformer.
 13. The device of claim 1, further comprising the primary focusing element.
 14. The device of claim 13, wherein the primary focusing element has an f-number that is greater than about 0.9.
 15. The device of claim 13, wherein the primary focusing element has an f-number that is greater than about 1.5.
 16. The device of claim 14, wherein the primary focusing element includes a Fresnel lens.
 17. The device of claim 16, wherein the Fresnel lens is flat.
 18. The device of claim 16, wherein the Fresnel lens is substantially square.
 19. The device of claim 16, wherein the Fresnel lens is curved.
 20. The device of claim 11, further comprising a means for homogenizing the light focused onto the entry aperture of the secondary concentrator.
 21. The device of claim 20, wherein the primary focusing element includes a diffractive lens.
 22. The device of claim 13, wherein the primary focusing element includes a Fresnel reflector.
 23. The device of claim 1, wherein the secondary concentrator has an f/number of 0.5 or less.
 24. The device of claim 1, wherein the secondary concentrator has an f/number of 1 or less.
 25. An apparatus for concentrating light from a source comprising: a truncated tapered reflector extending along an optic axis from a wide end to a narrow end and defining an interior region; and a concentrating lens mounted in the wide end of the reflector, said lens having a central region disposed about the optic axis and a peripheral region disposed about the central region; wherein the narrow end of the conical reflector is adapted to mount a receiver, wherein the concentrating lens is adapted to receive light from the source and concentrate light through the interior region and onto the receiver; wherein a portion of the light from the source passing through the central region of the concentrating lens is directed to the receiver without reflecting from the reflector; and wherein a portion of the light from the source passing through the peripheral region of the concentrating lens is reflected from a surface of the reflector facing the interior region and onto the receiver; wherein the concentrating lens is a comatic lens which is adapted to be substantially free from ray crossing at points about the optic axis proximal the narrow end of the reflector; and wherein the concentrating lens is characterized in that, in the absence of the reflector, each pair light rays entering the lens parallel to the optic axis and at differing radial distances from the optic axis are directed without crossing to a plane extending transverse the optic axis at a position corresponding to the position of the receiver at the narrow end of the reflector. 